JPH02129977A - Gas laser oscillator - Google Patents
Gas laser oscillatorInfo
- Publication number
- JPH02129977A JPH02129977A JP28248488A JP28248488A JPH02129977A JP H02129977 A JPH02129977 A JP H02129977A JP 28248488 A JP28248488 A JP 28248488A JP 28248488 A JP28248488 A JP 28248488A JP H02129977 A JPH02129977 A JP H02129977A
- Authority
- JP
- Japan
- Prior art keywords
- discharge electrode
- insulation plate
- discharge
- laser oscillator
- laser gas
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
- 239000000463 material Substances 0.000 abstract description 5
- 229910052751 metal Inorganic materials 0.000 abstract description 4
- 239000002184 metal Substances 0.000 abstract description 4
- 238000009413 insulation Methods 0.000 abstract 5
- 238000012216 screening Methods 0.000 abstract 4
- 229910000831 Steel Inorganic materials 0.000 description 3
- 238000005192 partition Methods 0.000 description 3
- 239000010959 steel Substances 0.000 description 3
- 229910052782 aluminium Inorganic materials 0.000 description 2
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 2
- 238000001816 cooling Methods 0.000 description 2
- 239000000498 cooling water Substances 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 1
- 239000003795 chemical substances by application Substances 0.000 description 1
- 239000012212 insulator Substances 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
- H01S3/09—Processes or apparatus for excitation, e.g. pumping
- H01S3/097—Processes or apparatus for excitation, e.g. pumping by gas discharge of a gas laser
- H01S3/0975—Processes or apparatus for excitation, e.g. pumping by gas discharge of a gas laser using inductive or capacitive excitation
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Engineering & Computer Science (AREA)
- Plasma & Fusion (AREA)
- Optics & Photonics (AREA)
- Lasers (AREA)
Abstract
Description
【発明の詳細な説明】
〔発明の目的〕
(産業上の利用分野)
本発明は、とくに高3周波電圧を放電電極間に印加して
発振させるガスレーザ発振器に関する。DETAILED DESCRIPTION OF THE INVENTION [Object of the Invention] (Industrial Application Field) The present invention particularly relates to a gas laser oscillator that oscillates by applying a high three-frequency voltage between discharge electrodes.
(従来の技術)
高周波電源を使った従来のガスレーザ発振器の一例を示
す第4図において、断面長方形の鋼板製の外部風洞1内
には、内部が外気に通じた断面U形の鋼板製の内部風洞
2が設けられ、外部風洞1の上部中央は石英ガラスなど
の絶縁板7Aが気密に取付られ、内部風洞2の上部にも
同じ絶縁板7Bが気密に取付られて、この二つの風洞間
には約601orrの圧力で封入されたレーザガスが下
部左側の送風機4で矢印3A、 3Bのように時計方向
に循環され下部右側の冷却器5で冷やされている。(Prior Art) In FIG. 4, which shows an example of a conventional gas laser oscillator using a high-frequency power source, an external wind tunnel 1 made of a steel plate with a rectangular cross section has an interior made of a steel plate with a U-shaped cross section that communicates with the outside air. A wind tunnel 2 is provided, and an insulating plate 7A made of quartz glass or the like is airtightly attached to the upper center of the outer wind tunnel 1, and the same insulating plate 7B is airtightly attached to the upper part of the inner wind tunnel 2, so that there is no air between these two wind tunnels. Laser gas sealed at a pressure of about 601 orr is circulated clockwise as shown by arrows 3A and 3B by a blower 4 on the lower left side and cooled by a cooler 5 on the lower right side.
又、絶縁板7Aの中央上面には放電電極板6Aが、絶縁
板7Bの中央下面には放電電極板6Bが取付られ、放電
電極6Aは高周波電源8の片側に、放電電極6Bは接地
された高周波電源の他側に接続されて絶縁板7A、 7
Bの内面間で放電させて紙面直交方向にレーザ光10を
発生させている。Further, a discharge electrode plate 6A is attached to the upper center surface of the insulating plate 7A, and a discharge electrode plate 6B is attached to the lower center surface of the insulating plate 7B, and the discharge electrode 6A is connected to one side of the high frequency power source 8, and the discharge electrode 6B is grounded. Insulating plate 7A, 7 connected to the other side of the high frequency power supply
A discharge is caused between the inner surfaces of B to generate laser light 10 in a direction perpendicular to the plane of the paper.
(発明が解決しようとする課題)
このように構成された高周波ガスレーザ発振器では、絶
縁板6^、6Bは内外の圧力差に耐える厚い材料が使わ
れており、それだけ放電電極6A、 68間に印加され
る電圧も高い電圧が要る。すると、放電電極6Bと内部
風洞2との所要沿面距離が増えて絶縁板7Bの幅も増え
るので、内部風洞2が大形となるだけでなく、耐圧上絶
縁板7A、 7Bの材料もより誘電率の高いものが要る
。(Problem to be Solved by the Invention) In the high-frequency gas laser oscillator configured in this manner, the insulating plates 6^, 6B are made of a thick material that can withstand the pressure difference between the inside and outside, and the voltage applied between the discharge electrodes 6A, 68 is increased accordingly. A high voltage is also required. Then, the required creepage distance between the discharge electrode 6B and the internal wind tunnel 2 increases, and the width of the insulating plate 7B also increases, so not only does the internal wind tunnel 2 become larger, but also the material of the insulating plates 7A and 7B becomes more dielectric in terms of voltage resistance. I need something with a high rate.
更に第5図に示すように絶縁板7Bと放電電極6B間に
できた微小な隙間Gで放電しレーザ発振器の効率を落と
す。Furthermore, as shown in FIG. 5, discharge occurs in the minute gap G formed between the insulating plate 7B and the discharge electrode 6B, reducing the efficiency of the laser oscillator.
そこで本発明の目的は、小形で効率のよい高周波放電の
ガスレーザ発振器を得ることである。SUMMARY OF THE INVENTION Therefore, an object of the present invention is to obtain a small and efficient high-frequency discharge gas laser oscillator.
(課題を解決するための手段と作用)
本発明は、対向面に低圧のレーザガスが循環され高周波
電源に接続された電極板が外面に取付られ両側が風洞壁
に取付けられた平行な一対の絶縁板間で放電電極させて
レーザガスを励起させる高周波ガスレーザ発振器におい
て、少くとも一側の放電電極を風洞内に設け、少くとも
一側の絶縁板の放電電極取付面に導電性の金属層を設け
ることで、外形が小形で発振器の効率をあげた高周波放
電のガスレーザ発振器である。(Means and Effects for Solving the Problems) The present invention provides a pair of parallel insulators in which low-pressure laser gas is circulated on opposing surfaces, electrode plates connected to a high-frequency power source are attached to the outer surfaces, and both sides are attached to the wind tunnel wall. In a high-frequency gas laser oscillator in which a laser gas is excited by a discharge electrode between plates, at least one discharge electrode is provided in a wind tunnel, and a conductive metal layer is provided on the discharge electrode mounting surface of at least one insulating plate. This is a high-frequency discharge gas laser oscillator with a small external size and increased oscillator efficiency.
(実施例)
以下、本発明の高周波放電のガスレーザ発振器の一実施
例を図面を参照して説明する。但し、第4図と重複する
部分は省く。(Embodiment) Hereinafter, one embodiment of the high-frequency discharge gas laser oscillator of the present invention will be described with reference to the drawings. However, parts that overlap with Figure 4 are omitted.
第1図において、絶縁板7Bの左右端の下面には、送風
機4間に鋼板製の仕切壁12Aが、冷却器5間に仕切壁
12Bが設けられてこの仕切壁12A、 12B間は冷
却器5で冷やされ送風機4で矢印3A、 3Bで示す時
計方向に循環されるレーザガスの流路の一部となってい
る。In FIG. 1, a steel plate partition wall 12A is provided between the blowers 4 and a partition wall 12B between the coolers 5 on the lower surface of the left and right ends of the insulating plate 7B. It forms part of a flow path for laser gas that is cooled by a blower 5 and circulated clockwise as shown by arrows 3A and 3B.
又、絶縁板7Bの放電電極6Bが接する面には、その部
分拡大図の第2図に示すように、アルミニウムの溶射層
11が予め形成されて放電電極6Bとは微小な空隙12
間にできた微小な突起部6B1で接しており、放電電極
6Bには冷却水を流す図示しない貫通穴が設けられてい
る。Further, as shown in FIG. 2, which is a partially enlarged view, on the surface of the insulating plate 7B that is in contact with the discharge electrode 6B, a sprayed aluminum layer 11 is formed in advance, and the discharge electrode 6B is separated from the discharge electrode 6B by a minute gap 12.
They are in contact with each other through a minute projection 6B1 formed between them, and the discharge electrode 6B is provided with a through hole (not shown) through which cooling water flows.
このような構成のガスレーザ発振器では、絶縁板IBの
上下の面はいづれも外部風洞1内のレーザガス圧の同一
圧力面となるので、板厚を薄くすることができる。する
と、高周波電源8で放電電極6A、 6B間に印加され
る電圧の周波数を落とす(例えば従来の数十MH2から
100M HZを数MH2に)ことができるだけでなく
、誘電率の高い材質でなくても仕切板12A、 12B
との耐電圧を保てるので、絶縁板7Bの材料の選定が容
易となり、幅を狭くできるので外部風洞1を小形にする
ことができる。In the gas laser oscillator having such a configuration, the upper and lower surfaces of the insulating plate IB are both at the same pressure surface of the laser gas pressure in the external wind tunnel 1, so that the plate thickness can be reduced. Then, not only can the frequency of the voltage applied between the discharge electrodes 6A and 6B by the high frequency power source 8 be lowered (for example, from the conventional several tens of MH2 to 100 MHz to several MH2), but also it is possible to reduce the frequency of the voltage applied between the discharge electrodes 6A and 6B. Also partition plates 12A, 12B
Since the withstand voltage can be maintained, the material for the insulating plate 7B can be easily selected, and the width can be made narrower, so the external wind tunnel 1 can be made smaller.
同様に、放電電極6A、68間に印加される高周波電圧
の周波数を落とすことで、電源から電極までの配線のり
アクタンスが減るので、電圧降下が減るだけでなく配線
が容易となる。Similarly, by lowering the frequency of the high-frequency voltage applied between the discharge electrodes 6A and 68, the wiring actance from the power source to the electrodes is reduced, which not only reduces voltage drop but also facilitates wiring.
更に、絶縁板7Bと放電電極68間の放電がなくなるの
で、レーザ発振器の効率を上げることができる。Furthermore, since there is no discharge between the insulating plate 7B and the discharge electrode 68, the efficiency of the laser oscillator can be improved.
なお、上記実施例において、放N電極6Aの外側に間隙
を介して絶縁板IAを覆う外壁を設けて放電電極6Aと
絶縁板7Aの外面もレーザガス内に入れてもよい。これ
により、絶縁板7Aの幅を狭くできレーザ発振器の外形
を更に小形化することができる。In the above embodiment, an outer wall may be provided outside the discharge electrode 6A to cover the insulating plate IA with a gap therebetween, so that the outer surfaces of the discharge electrode 6A and the insulating plate 7A are also placed in the laser gas. Thereby, the width of the insulating plate 7A can be narrowed, and the outer shape of the laser oscillator can be further reduced in size.
第3図は本発明の高周波放電のガスレーザ発振器の他の
実施例を示す。FIG. 3 shows another embodiment of the high frequency discharge gas laser oscillator of the present invention.
第3図においては、レーザ電源の接地例はアルミニウム
の溶射層11に直接接続されており、その外側に冷却部
13が取付られている。そして冷却部13には冷却水を
流す図示しない貫通穴が設けられている。In FIG. 3, the grounding example of the laser power source is connected directly to the sprayed aluminum layer 11, with the cooling section 13 mounted on the outside thereof. The cooling unit 13 is provided with through holes (not shown) through which cooling water flows.
〔発明の効果〕
以上、本発明によれば、平行に設けられた一対の絶縁板
の外面に高周波電圧が印加される放電電極板が取付られ
、絶縁板間に循環される低圧のレーザガスを励起して放
電させ、る高周波ガスレーザ発振器において、少なくと
も一側の絶縁板の放電電極をレーザガス室中に設け、少
なくとも一側の絶縁板の放電電極取付面に導電性の金属
層を設けたので、小形で効率のよい高周波放電のガスレ
ーザ発振器を得ることができる。[Effects of the Invention] As described above, according to the present invention, a discharge electrode plate to which a high frequency voltage is applied is attached to the outer surface of a pair of parallel insulating plates, and a low-pressure laser gas circulated between the insulating plates is excited. In a high-frequency gas laser oscillator that generates a discharge, the discharge electrode of at least one side of the insulating plate is provided in the laser gas chamber, and a conductive metal layer is provided on the discharge electrode mounting surface of at least one side of the insulating plate, so that it can be compact. It is possible to obtain an efficient high-frequency discharge gas laser oscillator.
第1図は本発明の高周波放電のガスレーザ発娠器の一実
施例を示す図、第2図は第1図の部分拡大図、第3図は
本発明の高周波放電のガスレーザ発振器の他の実施例を
示す図、第4図は従来の1周波放電のガスレーザ発振器
の一例を示す図、第5図は第4図の部分拡大図である。
1・・・外部風洞
6A、 613・・・放電電極
7A、 7B・・・絶縁板
8・・・高周波電源
11・・・金属溶射層
(8733) 代理人 弁理士 猪 股 祥 晃(ほ
か1名)
第
図
第
図FIG. 1 is a diagram showing one embodiment of the high-frequency discharge gas laser oscillator of the present invention, FIG. 2 is a partially enlarged view of FIG. 1, and FIG. 3 is another embodiment of the high-frequency discharge gas laser oscillator of the present invention. FIG. 4 is a diagram showing an example of a conventional single-frequency discharge gas laser oscillator, and FIG. 5 is a partially enlarged view of FIG. 4. 1...External wind tunnel 6A, 613...Discharge electrodes 7A, 7B...Insulating plate 8...High frequency power source 11...Metal sprayed layer (8733) Agent: Yoshiaki Inomata, patent attorney (and 1 other person) ) Figure Figure
Claims (1)
の絶縁板の外面中央部に高周波電圧が印加される放電電
極板が密着して取付られ、前記放電電極板間の高周波放
電で前記一対の絶縁板間を流れる低圧のレーザガスを励
起させるガスレーザ発振器において、 前記一対の絶縁板の少なくとも片側の前記放電電極取付
側を前記レーザガスが密封された前記風洞内に設け、前
記一対の絶縁板の少なくとも片側の前記放電電極取付面
に導電層を形成したことを特徴とするガスレーザ発振器
。[Scope of Claims] A discharge electrode plate to which a high frequency voltage is applied is closely attached to the center of the outer surface of a pair of parallel insulating plates whose outer peripheries are airtightly attached to the wind tunnel wall, and between the discharge electrode plates In a gas laser oscillator that excites low-pressure laser gas flowing between the pair of insulating plates with a high-frequency discharge, at least one side of the pair of insulating plates on which the discharge electrode is attached is provided in the wind tunnel in which the laser gas is sealed; A gas laser oscillator characterized in that a conductive layer is formed on the discharge electrode mounting surface of at least one side of a pair of insulating plates.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP28248488A JPH02129977A (en) | 1988-11-10 | 1988-11-10 | Gas laser oscillator |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP28248488A JPH02129977A (en) | 1988-11-10 | 1988-11-10 | Gas laser oscillator |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH02129977A true JPH02129977A (en) | 1990-05-18 |
Family
ID=17653038
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP28248488A Pending JPH02129977A (en) | 1988-11-10 | 1988-11-10 | Gas laser oscillator |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH02129977A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH06120591A (en) * | 1992-10-05 | 1994-04-28 | Mitsubishi Electric Corp | Laser oscillator |
JP2002185062A (en) * | 2000-12-14 | 2002-06-28 | Amada Eng Center Co Ltd | Ac discharge gas laser oscillator |
-
1988
- 1988-11-10 JP JP28248488A patent/JPH02129977A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH06120591A (en) * | 1992-10-05 | 1994-04-28 | Mitsubishi Electric Corp | Laser oscillator |
JP2002185062A (en) * | 2000-12-14 | 2002-06-28 | Amada Eng Center Co Ltd | Ac discharge gas laser oscillator |
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